Trust what you hear, your perceptions are unique to you.
1) Select active devices for minimum upper harmonic distortion. Although some devices have reasonably low second-harmonic distortion, the ear is not very sensitive to 2nd harmonic. It's the 3rd and higher-order harmonics that create unpleasant "electronic" colorations. D.E.L. Shorter of the BBC Research Labs and Norman Crow Hurst both proposed weighting harmonics by the square or cube of the order in to reflect audibility and annoyance-factor, and it's a shame their suggestions were never carried out. To this day, it's the 2nd harmonics that dominates THD device measurements, but it's the ones that are higher than that (even though they may be 20dB lower) that we hear. That's why a THD spec, without reference to the complete spectrogram, is essentially useless, and not only that, potentially quite misleading. In the absence of a full spectrogram, try and find a 2nd and 3rd-harmonic spec for the device you're interested in. It should be at least 20 to 30dB lower than the dominant 2nd-order distortion term. Failing that, there are some devices to avoid if you want to minimize the proportions of high-order harmonics - pentodes, beam tetrodes, transistors, MOSFETs, and IGBTs. That leaves triodes, which are not all the same.
The triodes that were the most popular in the Fifties (12AX7, 12AU7, 12AT7, and 6DJ8) were not in fact the most linear available. At the time, commercial amplifiers used at least 20dB of feedback, giving no incentive to retain big, old-fashioned octal tubes like the 6SN7 (size mattered back then). The 6SN7 came out of a prewar family of medium-mu radio tubes, starting with the single triodes 27, 37, 56, 76, 6P5, 6C5, 6J5, and then, the dual-triode 6SN7, introduced in 1940.
The 6SN7, used in millions of radios and early black-and-white TV sets, was replaced by the 12AU7 miniature tube in the early Fifties. Although the electrical characteristics appear identical in a databook (Rp=7700 ohms, mu=20), the 12AU7 has quite a bit more distortion than it's octal predecessor. In fact, the 6FQ7 miniature was introduced as a direct-replacement for the 6SN7, carrying forward the low-distortion characteristics of the 6SN7, but saw very little use in Fifties hifi equipment as a result of higher cost.
Tubes in widespread use in the Fifties have acquired a "cult" status that has nothing to do with performance, or even sonics. Believe it or not, there were better tubes both earlier and later than the "Golden Age" favorites. The 6SN7 and it's predecessors have very low distortion, almost certainly because they were designed before widespread use of feedback.
The Space Age high-transconductance tubes of the late Fifties and early Sixties never saw use in commercial hifi equipment, mostly due to cost considerations. But commercial and aerospace-grade tubes were some of the best ever made for low distortion - and favorable distribution of harmonics. The 5687, 6900, 7044, and 7119 are at the head of the line for low output impedance, wide voltage swing capability, high current, and low distortion. As for modern tubes in the same family, I've heard good things about the Sovtek 6N6 and 6H30.
Speaking of exotic, for brave souls who aren't afraid of microphonics or 50 MHz oscillations, there's the exotic (and hard-to-use) WE417A/Raytheon 5842, and the truly over-the-top WE437 or 3A/167M. (Available in modern form as the Russian 6C45pi.) Beware of large sample variations (20% or more) in this family - it's very hard to get matched pairs unless you burn them in for 100 hours and then re-test for gain. It isn't that quality is bad - the same problem is seen in genuine Western Electric 437's - it's that ultrahigh transconductance specifications requires extremely close-tolerance manufacturing. By comparison, the more moderately specified 5687, 6900, 7044, 7119, and ECC99 family is typically quite well matched, with variations of less than 5% from sample to sample.
2) Design circuits that optimize the linearity of the active device. For triodes, this means active, choke, or transformer loads. RC-coupling, although essential for the extended HF bandwidth required by feedback circuits (like the Williamson, Dynaco, or Marantz), degrades the distortion of triodes anywhere from 2 to 4 times relative to active, choke, or transformer loads.
An additional advantage of no RC coupling between the driver and output tubes is instant recovery from overload. RC coupling usually requires hundreds of milliseconds to recover the correct bias point for the output tubes. This is great for guitar amps, not so good for hifi applications, where immediate recovery is much more desirable.
3) Zero feedback in either local or global circuits. Some would say all triodes have large amounts of local feedback, but I would say, take a close look at the ratio of upper to lower harmonics. For the lower-order harmonics (2nd and 3rd), you'll see a reduction in direct proportion to the amount of feedback. But feedback generates harmonics of its own, in small magnitudes perhaps, but in greatly increased order. A classic article by Crowhurst mathematically demonstrates that a non-feedback amplifier with 9th-order harmonics acquires 81st-orderharmonics when feedback is added. So feedback, while substantially reducing lower-order harmonics (the most sonically benign), also creates entirely new high-order harmonics (albeit at very low magnitudes).
So if the theory of triodes having large amounts of local feedback is correct, they'd have less distortion at low orders of harmonic distortion than pentodes, but more distortion at higher orders. This is exactly the opposite of what measurements disclose. Measurements going back as far Harry F. Olson (see below) show triodes not only have less distortion overall, but most significantly, have far less upper-harmonic distortion. In fact, vanishing amounts of upper-harmonic distortion is the distinctive hallmark of triodes, compared to all other amplifying devices.
The exceptional linearity of Class A triodes removes the need for feedback in the first place, sidestepping problems with phase margin and stability with complex and nonlinear loads ... which pretty much describes all loudspeakers. In particular, complex back-EMF currents from the drivers stop at the plates of the output tubes, instead of being mixed at the summing node with the incoming signal. This avoids load-dependent distortion terms being generated in the feedback circuit.
4) Generous driver design. Most commercial tube amps only have 1 or 2dB of headroom in the driver circuit, so the entire amp clips at once. This leads to longer recovery times and exaggerating the audibility of clipping. I prefer 3 to 6dB of headroom, so the driver can retain its (voltage) linearity even when the output stage is deep into clipping.
Perhaps more important is adequate current and low output impedance in the driver. Much of the amplifier coloration is actually in the driver, and is a result of not enough current to properly charge the grids of the output tubes. I give Arthur Loesch credit for pointing out that the "sound" of different DHT output tubes is greatly exaggerated by not having enough current in the driver. With enough current, DHT's become more transparent sounding and begin to lose the characteristic colorations they are known for. This implies that grid current is present during much of the duty cycle and is quite nonlinear. The more current available and the lower the source impedance, the less important this grid-current nonlinearity will be.
The capacitive load the output tube presents to the driver changes the load-line into an ellipse, which pushes the driver into it's nonlinear low-current region - once per cycle for a SE amp, twice per cycle for a PP amp. Pentodes have both less capacitance and half - or less - the voltage requirements of DHT's, so the driver requirements are relaxed (EL84's are particularly easy to drive, needing only 10 volts). DHT's, on the other hand, are much more severe loads, more capacitive, needing twice the voltage swing, and worst of all, exposing the driver distortion since DHT's have such low intrinsic distortion of their own. The sad fact is that many commercial DHT amplifiers, certainly all the RC-coupled designs, have more distortion in the driver than the output tube! What's the point in spending hundreds of dollars on a handmade 45, 2A3, 300B, or 845 if all you hear is the driver distortion? But that's why DHT sound quality is all over the place - the driver section isn't up to the job.
5) Absence of rectifier switching noise. The noisiest circuits of all are solid-state bridges driving large values of electrolytic capacitors. (As found in almost all transistor gear and the DC supplies for heaters and filaments.)
The commutation noise of the diodes shock-excites the RLC of the stray L in the cap bank and the stray C in the power trans secondary. The resonance of this tank circuit is typically anywhere from 4 to 20KHz and the Q's are large, anywhere from 5 to 100, depending on the DCR of the caps. This is why paralleling large values of electrolytic with "better", faster polypropylenes can frequently result in worse sound. It is also the reason power cables are audible ... they act as antennas for the small Tesla coil that most power supplies resemble. The supply radiates noise into the chassis, the power supply B+ lines, the audio circuit, and the power cable. This broadband noise can be filtered and shielded (at considerable trouble), but it is much easier to eliminate the commutation switch-noise right at the source.
Choke-fed supplies are much quieter due to the choke slowing down the rate-of-charge of the main cap bank. I use a hybrid choke-fed/pi-filter to minimize the shock-excitation of the main PS choke (this tip from the Radiotron Designers Handbook, Fourth Edition).
In terms of ragged waveforms, solid-state diodes are the worst, followed by Schottky diodes and HEXFRED's, followed by conventional tube rectifiers, followed by TV damping diodes, which are the smoothest of all in terms of the AC waveform on the power trans secondary. This, along with 2 amp peak current, is why I use them. The 30 second warm-up is just a bonus.
Trust what you hear; people really do hear different things, and your perceptions are unique to you. I've been in high-end audio for thirty years now, and I've only found a handful of people who hear things the same way I do. Audio perceptions are every bit as individual as food preferences or your idea of the best lover or life companion; why should you take the guidance of a stranger you've never met? Listen for yourself, get out of the stores and hi-fi shows, and hear what's going on with the more adventurous builders. You'll be surprised.
Chief Designer of INCRECABLE Acoustic Lab
2018 New NEVE DCT3 Speaker Cable is coming!!
New BASSO Speaker Cable is coming!!
2017 New IPC-6GB Power Clearifier is available now!
2017 New iBLOCK MVD-1 Vibration Decoupler is available now!
2017 New SOLO Centre Speaker Cable is available!
2017 New RAINFOREST Speaker Cable is available!
2017 New iGROUND Grounding Cable is available!
2017 New iJUMP Loudspeaker jumper link is available!
iAMP's TIA & TPA series are available!
iUSE Silver Plated 6N OFHC HD-USB Cable is available!
iWATCH New 4K High Speed HDMI Cable
iSOUND 2017 New 6N OFHC Speaker Cable by Reel
TIME TUNNEL SKYDANCE
ILISTEN 2017 New 4N OFHC Interconnect Cable
CRYSTAL Twisted pair RCA & XLR audio interconnect are available NOW!
New 6N OFHC Digital Power Cord
LAVA Digital Power Cord Is available NOW!
New DCT3 SIP Power Cord
IPC-8 Power Clearifier is available now!
IEH-2 Energy Headquarter DCT Duplex Receptacle is available now!